Temperature regime in the surface layer of the substrate in the area under the evaporating liquid drop; International Communications in Heat and Mass Transfer; Vol. 169, Pt. C

Bibliografske podrobnosti
Parent link:International Communications in Heat and Mass Transfer.— .— Amsterdam: Elsevier Science Publishing Company Inc.
Vol. 169, Pt. C.— 2025.— Article number 109795, 18 p.
Drugi avtorji: Syrodoy S. V. Semen Vladimirovich, Kuznetsov G. V. Geny Vladimirovich, Tamashevich Maksim M., Zamaltdinov R. R. Roman Rinatovich, Voytkova K. A. Kseniya Arturovna, Bulba E. E. Elena Evgenievna, Kostoreva Zh. A. Zhanna Andreevna, Gutareva N. Yu. Nadezhda Yurievna, Solomatov V. V. Vladimir Vasiljevich
Izvleček:Title screen
The need to comply with the regulatory temperature regime in intensively heated elements of electronic and radio-electronic equipment leads to the search for methods of effective heat removal in such conditions. For this reason, much attention has been paid to the study of drop cooling systems for surfaces heated to high temperatures, in recent years. However, until recently, the analysis of drop cooling processes has been carried out without directly measuring the temperatures of the cooled element in the area of the coolant drop. In this case, the temperatures in the layer of heated material adjacent to the contact surface with the drop are the main characteristic of the operation of such a cooling system. The purpose of this work is to experimentally determine temperatures in a thin layer of material adjacent to the interface “drop of water – plate of heated metal” in a typical range of the changes in heat fluxes and temperatures of heated equipment elements. According to the experimental results, evaporation of a drop under conditions of its conductive heating by the surface of a plate with a temperature from 60C to 100C leads to a decrease in surface temperatures, which is the interface “drop – heated plate” by no more than 1–3C. In other words, a drop can provide a regime close to a constant temperature of the heated surface, but not significantly reduce it. It has also been found that the temperature of the open surface of the plate differs slightly (by 2–3C) from the temperature of the surface on which the drop is located. A hypothesis is formulated about the mechanism of the established effect: a slight decrease in the temperature of the surface layer of the plate in the area covered by the drop is due to the flow of heat in two transverse coordinate directions from zones that are not affected by evaporation of the drop beyond the reach of its boundaries
Текстовый файл
AM_Agreement
Jezik:angleščina
Izdano: 2025
Teme:
Online dostop:https://doi.org/10.1016/j.icheatmasstransfer.2025.109795
Format: Elektronski Book Chapter
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=683797

MARC

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200 1 |a Temperature regime in the surface layer of the substrate in the area under the evaporating liquid drop  |f S. V. Syrodoy, G. V. Kuznetsov, M. S. Tamashevich [et al.] 
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330 |a The need to comply with the regulatory temperature regime in intensively heated elements of electronic and radio-electronic equipment leads to the search for methods of effective heat removal in such conditions. For this reason, much attention has been paid to the study of drop cooling systems for surfaces heated to high temperatures, in recent years. However, until recently, the analysis of drop cooling processes has been carried out without directly measuring the temperatures of the cooled element in the area of the coolant drop. In this case, the temperatures in the layer of heated material adjacent to the contact surface with the drop are the main characteristic of the operation of such a cooling system. The purpose of this work is to experimentally determine temperatures in a thin layer of material adjacent to the interface “drop of water – plate of heated metal” in a typical range of the changes in heat fluxes and temperatures of heated equipment elements. According to the experimental results, evaporation of a drop under conditions of its conductive heating by the surface of a plate with a temperature from 60C to 100C leads to a decrease in surface temperatures, which is the interface “drop – heated plate” by no more than 1–3C. In other words, a drop can provide a regime close to a constant temperature of the heated surface, but not significantly reduce it. It has also been found that the temperature of the open surface of the plate differs slightly (by 2–3C) from the temperature of the surface on which the drop is located. A hypothesis is formulated about the mechanism of the established effect: a slight decrease in the temperature of the surface layer of the plate in the area covered by the drop is due to the flow of heat in two transverse coordinate directions from zones that are not affected by evaporation of the drop beyond the reach of its boundaries 
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461 1 |t International Communications in Heat and Mass Transfer  |c Amsterdam  |n Elsevier Science Publishing Company Inc. 
463 1 |t Vol. 169, Pt. C  |v Article number 109795, 18 p.  |d 2025 
610 1 |a Water drop 
610 1 |a Substrate 
610 1 |a Heat flow 
610 1 |a Evaporation 
610 1 |a Cooling 
610 1 |a Temperature fields 
610 1 |a электронный ресурс 
610 1 |a труды учёных ТПУ 
701 1 |a Syrodoy  |b S. V.  |c specialist in the field of thermal engineering  |c Professor of Tomsk Polytechnic University, Doctor of Technical Sciences  |f 1988-  |g Semen Vladimirovich  |9 18392 
701 1 |a Kuznetsov  |b G. V.  |c Specialist in the field of heat power energy  |c Professor of Tomsk Polytechnic University, Doctor of Physical and Mathematical Sciences  |f 1949-  |g Geny Vladimirovich  |9 15963 
701 1 |a Tamashevich  |g Maksim  |b M.  |f 1999-  |c specialist in the field of thermal power engineering and heat engineering  |c Engineer of Tomsk Polytechnic University  |9 88761 
701 1 |a Zamaltdinov  |b R. R.  |c specialist in the field of thermal power engineering and heat engineering  |c Engineer of Tomsk Polytechnic University  |g Roman Rinatovich  |f 1999-  |9 88705 
701 1 |a Voytkova  |b K. A.  |c specialist in the field of heat and power engineering  |c engineer assistant of Tomsk Polytechnic University  |f 1994-  |g Kseniya Arturovna  |9 23069 
701 1 |a Bulba  |b E. E.  |c specialist in the field of thermal engineering  |c Associate Professor of Tomsk Polytechnic University, Candidate of technical sciences  |f 1969-  |g Elena Evgenievna  |9 18330 
701 1 |a Kostoreva  |b Zh. A.  |c Specialist in the field of heat and power engineering  |c Engineer of Tomsk Polytechnic University  |f 1994-  |g Zhanna Andreevna  |y Tomsk  |9 22104 
701 1 |a Gutareva  |b N. Yu.  |c linguist  |c Associate Professor of Tomsk Polytechnic University, Candidate of pedagogical sciences  |f 1979-  |g Nadezhda Yurievna  |9 15274 
701 1 |a Solomatov  |b V. V.  |g Vladimir Vasiljevich 
801 0 |a RU  |b 63413507  |c 20251218 
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